We report the realization of a mid-infrared (lambda similar or equal to 7 mu m) quantum-cascade laser. in which the emission process takes place between the two lowest minibands of an intrinsic superlattice. Contrary to previous lasers based on doped superlattices, here the dopants are located only inside suitably designed injector regions, where positive ionized donors and negative electrons are arranged to compensate the applied external field across the superlattices. This reduces impurity scattering and translates into low threshold currents (4.2 kA/cm(2) at 10 K) and into room temperature operation, without compromising the large current-carrying capabilities of the minibands. Peak powers of similar to 1.3 W per facet have been obtained from broad-area devices at 10 K, with still more than 1 W at 120 K and 400 mW at 200 K. Effects related to the finite size of the superlattices become visible in the spectral properties, owing to the reduced broadening, and have to be taken into account to accurately describe the laser's behavior. [S0003-6951(98)04419-2].
High-power inter-miniband lasing in intrinsic superlattices
Tredicucci A;
1998
Abstract
We report the realization of a mid-infrared (lambda similar or equal to 7 mu m) quantum-cascade laser. in which the emission process takes place between the two lowest minibands of an intrinsic superlattice. Contrary to previous lasers based on doped superlattices, here the dopants are located only inside suitably designed injector regions, where positive ionized donors and negative electrons are arranged to compensate the applied external field across the superlattices. This reduces impurity scattering and translates into low threshold currents (4.2 kA/cm(2) at 10 K) and into room temperature operation, without compromising the large current-carrying capabilities of the minibands. Peak powers of similar to 1.3 W per facet have been obtained from broad-area devices at 10 K, with still more than 1 W at 120 K and 400 mW at 200 K. Effects related to the finite size of the superlattices become visible in the spectral properties, owing to the reduced broadening, and have to be taken into account to accurately describe the laser's behavior. [S0003-6951(98)04419-2].I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
